5G/NR - OTA
OTA (Over The Air)
OTA stands for Over The Air. In order to perform test a device with any test equipment, you need a way of connecting the device to the test equipment. OTA is a kind of method connecting a device to a test equipment. There are roughly two kinds of connection method as shown below. One is Conductive and the other one is Radiative (or OTA). Simply put, OTA is a connection method via a pair of antenna (Transmiting antenna and Recieving Antenna).
Actually OTA is a very complicated topic. There are many different aspect to think of. I will try to cover as many different perspective as possible as I learn and experience more.
When we say Radiative testing, it usually refers to various different types of configurations as shown below. These are just a few typical examples that you may see most often, but these are not all. There are so many different variations of Radiative Test Setups. Even though the terms OTA Test and Radiative Test can be used interchangeably, when we say OTA test without any specific details, we normaly think of the configuration like (C) or (D) shown below. As shown below, it is test in a chamber lined with absorbers (this kind of chamber is called Anechoic chamber. Anechoic means 'No Echo'. 'No Echo' in this case mean 'No reflection from any object in the box).
Even in conventional technologies (e.g, UMTS, LTE), sometimes we performed OTA measurement especially for TRP or TIS measurement. However, in 5G/NR we are talking about OTA with almost every test, even with protocol test. Why OTA has become such a big issue in 5G/NR ? In NR, there are roughly two separated spectrum that are specified in 3GPP specification. One is FR1 (sub 6 Ghz) and the other is FR2(mmWave). In FR1, we may continue to go with the conductive testing as we do with 2G/3G/4G technology. However, in FR2 it is highly likely that we are forced to go with OTA. Why ?
We can think of several reasons for this and with a few different aspect.
In order to get a repeatble, reliable and stable measurement result, it is very important to place the AUT(Antenna Under Test) and the measurement antenna in proper position. In this section, I will explain on how to determine the proper antenna position and theoretical background on why the specific posiiton should be used.
Minimum far-field distance R for a traditional far field anechoic chamber are determined by the formula a shown below (Based on R5-180013).
< Figure 1 : Antenna Field Region >
The near/far field boundary for different antenna sizes and frequencies is shown in the table below. This table is based on R5-180013 (Ref ) - Table 2.2.1: Near field/far field boundary for different frequencies and antenna sizes for a traditional far field anechoic chamber
< Table 1 - Near/Far Boundary distance with D and Frequency >
NOTE : From this is the optional reading. I've looked into the equation a little bit deeply just out of curiosity. If may skip this part if you are not interested. I tried to investigate on how the near / far boundaries changes as frequency changes.
As shown below, the span of Radiative Near Field (the gap between the end of Reactive Near Field and the Start of Far Field) gets drastically increases as frequency increases where as Reactive Near Field distance relatively slowly increases). Also, comparing the following two plots, you would notice that the Far Field distance gets drastically larger as D increases.
< Figure 2 - Field Boundary change with frequencies at D = 5 cm >
< Figure 3 - Field Boundary change with frequencies at D = 10 cm >
Now you may have an interesting question. According to the plots shown above, the distance between DUT antenna and equipment antenna should increase as frequency increases. That is, the size of Anechoic chamber should increases as frequency increases ? Isn't it counter intuitive to you ? Our common sense (our RF intuition) says the size of frequency dependent object tend to decrease as frequency increases.
How do we handle this conflict with our intuition and the plots show above ?
The solution lies in the fact that D is not a constant in realilty. In case of plots shown above, D has a fixed value regardless of frequency. But when we design an antenna, we usually decide D value(Antenna Aperture size) in terms wavelenth as shown below. Here, k is just a constant like 0.5, 1, 2 etc.
If you plot on how wavelength (lamda) changes as frequency increases, you will get a plot as shown below. You will notice that the wavelength decrease dtrastically.
< Figure 4 - Wavelength vs Freuqnecy >
If you rewrite Far Field distance equation, it becomes as shown below. In this equation, you will notice that the Far Field distance decreases as frequency increases. (NOTE : if you want to try calculate in real value, take f as 'frequency in Hz' and c as 'the speed of light in m', k is just a constant without any unit).
Probably by now, you may have a question 'Why do we need to test in Far Field ?'. It would not be easy to get a direct answer to this question. So let me change the question a little bit. Why we do not test in Near field ?
The simple answer to this question is that the measurement result in this region tend to be unpredictable and subject to change with small changes in the environment surrounding the antenna(e.g, electrical circuit feeding the antenna) and location changes. On the contrary, the field pattern in Far field is more stable and predictable and less senstive to small surrounding components.
For those who are interested in further details, let's look a little bit further details on the characteristics in each of the region. You may investigate even further on your own. Try googling the keywords like 'Near and Far Field', 'Field Region around Antenna' etc.
Reactive Near Filed : This is the area that is very close to the antenna. The relationship between E and H field in this region is very unpredictable (It is unpredictable not because this property goes against a physical theory, but because the physical property is so complicated). For example, at one point you would see E field dominates and at another point right besides the previous point H field dominates. Also radiated energy would influence back and forth with surrounding electrical component like antenna control circuit. For example, some portions of radiated energy gets absorbed and stored in surrounding component at some point of time and the stored energy gets radiated back into the space at other point of time and influence radiation pattern.
Radiative near field (Fresnel region) : In this region, the distance from the antenna is not so close to be influenced by reative electrical components as described above and the E and H field relationship is much more predictable comparing to Reactive Near Field. However, the E and H field relationship is still pretty complex and there are high possibilities where some physical object that may affect the radiation pattern in this area. For example, some metal object like steel beam holding up the antenna module can act as a kind of antenna or reflector. So this kind of object can influence on the radiation pattern of the AUT(Antenna Under Test).
FAR field (Fraunhofer region): In this region, the angular field distribution is essentially independent of the distance from the antenna and the radiation pattern can be approximated with spherical wave-fronts. Since any recieving point in the region are very far from the antenna, the transmitter size and shape are not important anymore and it can be approximated as a point source. The electric and magnetic fields are in phase, perpendicular to each other and perpendicular also to the direction of propagation. In this region, you can safely assume that the wave front going through the recieving antenna is planner (i.e, all the incoming rays are in parallel to each other). Putting it simple, this is the idea region in which most of measurement can be done easily and reliably.
As mentioned above, in order to achieve the stable measurement result it is important to put the distance between DUT antenna and the equipment antenna to be greater than the Far Field Boundary. As shound in [Figure 1], the Far Field boundary starts from the following distance.
As you notice from this expression, the distance is proportional to D squared (D represents antenna dimension). That is, the distance changes drastically with even a small changes in D. To give you more intuitive understanding, I plotted this equation in a graph as shown in left. The path loss at the boundary also increases as the D increases as shown in right.
< Figure 5 - Far Field Distance and Path Loss with D >
In case that you want to get the exact quantitative data, I put a table as shown below. The two graphs shown above are plotted from this table.
< Table 2 - D influencing on Far Field Distance and Path Loss >
What this implies is that you need to know the exact antenna dimension in order to get the accurate measurement. However, it is not always easy to correctly define the antenna dimension. Antenna Dimension D is defined as the maximum distance across the whole antenna module. The Red Arrow in [Figure 6] indicates D. As you see, it would be straightforward to define D in case of (A), (B), (C) and (E). However, in case of (D), defining the dimension would not be so easy. In (D), the physical dimension is same as (A), but you see some conductive material around the antenna module influence the radiation pattern of the antenna module. This may influence the effective dimension of the antenna and it would be very difficult to accurately estimate the effective dimension. Also there would be some possibilities where UE makers distribute the antenna modules accross several different locations inside of the UE as shown in (F), (G) and (H). Of course, the shape and location of Antenna modules within a UE would be more diverse and complicated than the ones shown here.
< Figure 6 - Antenna Dimensions for various configuration >
There is another reason why defining D gets difficult. It would get more difficult for UE case. In order to correctly define D, you need to have all the detailed information of the antenna structure and positions in UE. But in many cases these information is treated as a highly confidential information by most of UE manufacturer. So when you are given a UE (especially a commercialized UE), it is almost impossible to get the exact estimate for D (Dimension).
Now we are facing a very tricky situation. How can we guarantee the accurate measurement when we are not given the detailed information on Antenna dimension ?
This is what I will talk about next section.
Before getting into specific cases, let's think of the meaning of a few basic words - Whitebox and Blackbox. Whitebox refer to a box we can directly look into the box and clearly knows what is inside of the box. It means all the information about the box is known to ux. Blackbox refer to a box we have no direct visibility to the inside of the box. The only way that we can figure out the contents of the box is via indirect observation like shaking the box and listen to the sound or lifting up and estimate the weight etc. Of course, this is not the formal definition of Whitebox and Blackbox in OTA, but the basic idea applies to the formal definition as described in R4-1708553 (Ref ).
For the ”Black box” approach, the exact antenna locations/centre-of-Radiation-Reference-Point (CORRP) do not need to be known.
For the ”White box” approach, the exact antenna locations/centre-of-Radiation-Reference-Point (CORRP) need to be known, likely via a manufacturer declaration.
Now you may ask 'Why we are talking about whitebox / blackbox concept here ?' and 'how are they related to handling D(Antenna Dimension) ?'. Let's think of a situation where we have the detailed information on D and a situation where we don't have exact information on D.
Let's assume that we have all the detailed information about D. It means the Antenna module under test is a kind of whitebox. In this case, we can calculate the exact location of Near / Far boundary. Then we can get relatively accurate measurement with the minimum distance between DUT and Measurement Antenna(Probe) and still meeting the Far field criteria as in (A) of [Figure 6]. It means that we can meet the Far Field condition with minimum size of Anechoic chamber. In turn, it means we can get the accurate measurement with minimized cost on Anechoic chamber.
Now let's think of a situation where we don't have accurate information on D. How we can estimate the exact location of Near/Far boundary (i.e, Starting point of Far Field) ? The answer is 'There is no way to do it'. Then how we can guarantee that the antenna is in Far Field ? The simplest way is to place the receving antenna at a position which is very far away from the DUT so that you can assume that it is in Far field regardless of the size of antenna as in (B) of Figure 6. Of course there should be a certain limitation of Antenna size you assume. You would not assume that the antenna size is 20 cm when you have a mobile phone with the size of 10 cm.
< Figure 6 : Possible Antenna Location in Whitebox and Blackbox condition >
we may say if we can get the detailed information on Antenna dimension and exact antenna location on DUT (e.g, Mobile phone), it would be better to use Whitebox approach, since we can do the measurement with smaller chamber and at relatively low cost. This can be a good option at the development stage in which these informations tend to be open.
If the detailed information on Antenna dimesion and locations on Mobile phone, Blackbox approach will be the better option. Since most of the mobile phone manufacturer would be very reluctant to open the detailed information on antenna on their commercialized device, the blackbox approach may be the only option for the commercialized device. However, as mentioned above, we would need very large chamber to apply the blackbox approach which would cause cost and space issue. To mitigate this problem, an alternative concept were proposed and this alternative will be explained in next section.
NOTE : Regarding the adoption of Whitebox approach or Blackbox approach, Ref  states as follows :
For conformance testing, 3GPP has decided that only the black box approach can be used. This is due to the requirements for white box testing not being accepted by UE vendors who preferred not to declare the antenna structure.
As mentioned above, it is likely for only blackbox approach to be accepted as a test method for commercialized device since UE manufacturer does not like to disclose the detailed antenna information, but blackbox approach tend to require huge chamber (i.e, large distance between the transmitter and reciever antenna). To reduce the problem of the chamber size issue an alternative concept called CATR(Compact Area Test Range). The overall concept is described in TR 37.842 as shown below.
< TR 37.842 - Figure 10.3.1.1.3.1-1: CATR measurement system setup for EIRP >
As shown above, you will see the signal from the transmitter antenna bounces (reflects) from a specially designed reflector and then reaches to the receiver antenna. This would take an effect of folding up a long linear distance into a small space, which result in reducing the size of the chamber. In addition, by designining the reflector in a specific form, you can make all the parallel rays from DUT reaches to Feed antenna(measurement antenna). And, also you can make the rays from the feed antenna reaches DUT as parallel rays. Actually the basic principle is similar to what you learned in high school physics about Ray diagram of Parabolic mirror. Try googleing 'Parabolic Mirror Ray Diagram' or 'Parabolic Mirror Ray Tracing' etc.
The concept of SS MPAC is to use multiple probes around UE as illulstrated below to emulate more realistic radio channel condition.
< R4-1706669 : Figure 2. Installed probes in the sector and UE >
The major motivation of SS MPAC is well described in R4-1706669 as follows :
1. Real–time system performance assessment, i.e. while communicating
2. Capable of emulating realistic radio channels, meaning with realistic angular distributions of waves, either irradiating EU or being radiated by it
3. Up– and downlink performance, or reception and response in multi–node configurations
According to Ref , Quiet Zone is the volume in any chamber in which a DUT is illuminated with nearly uniform amplitude and phase. Typical quiet zone specifications are 10 degrees of phase variation, ± 0.5 dB of amplitude ripple, and 1 dB of amplitude taper, which is the roll-off toward the edges of the quiet zone
 3GPP TSG-RAN WG5 Adhoc Meeting#1 - R5-180013 : Signalling NR Testcases - OTA chamber requirements
 Keysight Technologies - OTA Test for Millimeter-Wave 5G NR Devices and Systems (White Paper)
 3GPP TSG-RAN WG4 Meeting #84 - R4-1708553 : Far field definition and proposal for alternate RF baseline with deterministic antenna array positioning
 3GPP TSG RAN WG4 Meeting NR#2 - R4-1706617 : Center of Radiation Reference Point – Reference Definition for OTA Measurements of Phased Array Beamforming Patterns
 3GPP TR 37.842 V13.2.0 (2017-03) - Radio Frequency (RF) requirement background for Active Antenna System (AAS) Base Station (BS)(Release 13)
 3GPP TSG-RAN WG4 Meeting NR AH#2 - R4-1706669 : SS MPAC for RRM/Demod
 TR 37.977 - Verification of radiated multi-antenna reception performance of User Equipment (UE)
 OTA Test for Millimeter-Wave 5G NR Devices and Systems (Keysight Whitepaper)
 3GPP TR 38.827 - Study on radiated metrics and test methodoloty for the verification of multi-antenna reception performance of NR User Equipment (UE).